quentin fouliard, sandip haldar, ranajay ghosh, seetha raghavan · 2019. 7. 12. · quentin...

1
The challenge with modeling Thermal Barrier Coating optical properties is to account for the significant amount of scattering that occurs due to the intrinsic inhomogeneities of porous ceramic materials that are used to lower thermal conductivities. In addition, it is necessary to consider absorption of light as it travels through the coating. A well-known model that combines both factors is the Kubelka-Munk model. The following equations are describing the distribution of intensities of excitation and emission lights as the laser beam penetrates TBC that contains luminescent dopants [2]: The model has been further extended to predict the luminescence coming from the thermally grown oxide (TGO) that forms when aging the material: Innovative specimens including dopant in the bond coat that diffuses to the thermally grown oxide are currently being prepared for temperature measurements at the top coat - bond coat interface. The monitoring of temperature at this key location can help controlling the degradation mechanisms occurring in operating conditions on turbine blades and allow for more efficient engines. One of the main work on this model is the integration of decay time for numerical predictions of the collectable 0, , in presence of a gradient of temperature based on the following equation: The equation includes the exponential decay that is characteristic of luminescence. The latter equation is providing very promising results to correlate temperature readings obtained with decay time phosphor thermometry and its accurate position in the coating, allowing for reduction of errors in the evaluation of the temperature distribution. Based on this results, a reverse model has been constructed to predict temperature at any point in the TBC using a single point measurement. The plot presented below show the results of equivalent position for the temperature measurement and collectable intensity using the model for 325 TBC layer configurations on YSZ:Dy The precision of the previous results is to be related to the effects of the input gradient of temperature on the model. The sensitivity of the model to the input surface temperature and internal gradient for the configuration (C1) for YSZ:Dy is shown below. It has been found that for the usable range of temperature of this material (800K–1450K) the equivalent position remains constant ( ±8K error) which allows to retrace temperature and internal gradients simply based on Phosphor Thermometry. Thermal barrier coatings (TBCs) are used to protect turbine components from the extremely hot gas ow, which may be above the component materials melting point. Accurate temperature measurements enable precise lifetime predictions, which favor safety and efficiency. In-situ monitoring of in-service turbine components is ideal; a promising method is Phosphor Thermometry which uses the luminescence decay of doped coatings stimulated by a pulsed laser. There are various congurations of candidate phosphors and host materials, but it is crucial to ensure both sensing and integrity needs are met. BACKGROUND & MOTIVATION METHOD : LUMINESCENCE DECAY MODELING COLLECTABLE LUMINESCENCE USING FOUR-FLUX KUBELKA-MUNK MODEL INTEGRATION OF DECAY TIME The Phosphor Thermometry instrumentation at the University of Central Florida has been constructed in collaboration with Dr. Heeg at Lumium, The Netherlands, and is composed of a switchable 355 nm / 532 nm wavelength pulsed laser that excites doped specimens. Neutral density and bandpass filters are used to collect the luminescence. A photomultiplier tube is used to convert the photons into a detectable electric signal. The data collection is then processed through MATLAB. The sensitivity of the temperature measurement is proper to each configuration and based on the variation of decay time with temperature. The equipment has been designed so it is adaptable to the sample positioning and portable. REFERENCES & ACKNOWLEDGMENTS [1] Fouliard, Q. P., Jahan S. A., Rossman L., Warren P., Ghosh R., Raghavan S., Configurations for Temperature Sensing of Thermal Barrier Coatings, International Conference on Phosphor Thermometry, 25-27 July, 2018, Glasgow, UK [2] Fouliard, Q. S. Haldar, R. Ghosh, S. Raghavan, Modeling Luminescence Behavior for Phosphor Thermometry Applied to Doped Thermal Barrier Coating Configurations, Applied Optics (2019) - Submitted [3] Pilgrim, C. C., J. P. Feist, and A. L. Heyes. "On the effect of temperature gradients and coating translucence on the accuracy of phosphor thermometry." Measurement Science and Technology 24.10 (2013): 105201. This material is based upon work supported by the U.S. Department of Energy, National Energy Technology Laboratory, University Turbine Systems Research (UTSR) under Award Number: DE- FE00312282. Sensing TBC configurations have been separated into two categories: (C1) is easier to manufacture, does not add any extra interface and provides higher luminescence intensities. (C2) gives higher accuracy of luminescence signal [1]. Department of Mechanical and Aerospace Engineering, College of Engineering and Computer Science, University of Central Florida, Orlando, Florida, USA Quentin Fouliard, Sandip Haldar, Ranajay Ghosh, Seetha Raghavan OBJECTIVES DOPED LAYER TBC CONFIGURATIONS Data collection through doped TBCs at high temperature. Addition of a PMT with a different bandpass configuration for the combination of the decay and the intensity ratio methods. Specimen fabrication and residual strain characterization of the doped TBCs to ensure the mechanical integrity of the specimens. Quantify the luminescence intensity for any TBC configuration. Predict the location into the TBC of the Phosphor Thermometry temperature output. INSTRUMENTATION Fan Low-Pressure Compressor High-Pressure Compressor Combustor Low- Pressure Turbine High- Pressure Turbine & Coated Blade Thermal Barrier Coating Image courtesy: GE FUTURE WORK MATERIALS YSZ:Eu (1% Eu 2 O 3 , 8% Y 2 O 3 , 91% ZrO 2 ) TBC coupons were prepared by Air Plasma Spray at the Florida Institute of Technology to validate initial results of Kubelka-Munk based models. Er, Dy, Sm and Cr dwdadw 250 μm Doped top coat Undoped top coat Bond coat Substrate (C1) (C2) Thermally grown oxide are other dopants that will be made for Phosphor Thermometry. This instrument is combined with an infrared heater (model E4 from Precise Control Systems Inc, MN, USA) that is capable of heating the specimens up to 1300˚C to reproduce TBC real service conditions. Measurements have been taken on YSZ:Eu powder and a fit allows for retracing temperature. YSZ:Eu top coated sample

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Page 1: Quentin Fouliard, Sandip Haldar, Ranajay Ghosh, Seetha Raghavan · 2019. 7. 12. · Quentin Fouliard, Sandip Haldar, Ranajay Ghosh, Seetha Raghavan OBJECTIVES DOPED LAYER TBC CONFIGURATIONS

The challenge with modeling

Thermal Barrier Coating optical

properties is to account for the

significant amount of scattering

that occurs due to the intrinsic

inhomogeneities of porous ceramic

materials that are used to lower

thermal conductivities. In addition,

it is necessary to consider

absorption of light as it travels

through the coating. A well-known

model that combines both factors

is the Kubelka-Munk model. The

following equations are describing

the distribution of intensities of

excitation and emission lights as

the laser beam penetrates TBC that

contains luminescent dopants [2]:

The model has been further

extended to predict the

luminescence coming from the

thermally grown oxide (TGO) that

forms when aging the material:

Innovative specimens including

dopant in the bond coat that

diffuses to the thermally grown

oxide are currently being prepared

for temperature measurements at

the top coat - bond coat interface.

The monitoring of temperature at

this key location can help

controlling the degradation

mechanisms occurring in operating

conditions on turbine blades and

allow for more efficient engines.

One of the main work on this

model is the integration of decay

time for numerical predictions of

the collectable 𝐽𝑙𝑢𝑚 0, 𝑡 , in presence

of a gradient of temperature

based on the following equation:

The equation includes the

exponential decay that is

characteristic of luminescence. The

latter equation is providing very

promising results to correlate

temperature readings obtained

with decay time phosphor

thermometry and its accurate

position in the coating, allowing

for reduction of errors in the

evaluation of the temperature

distribution. Based on this results,

a reverse model has been

constructed to predict temperature

at any point in the TBC using a

single point measurement.

The plot presented below show the

results of equivalent position for

the temperature measurement and

collectable intensity using the

model for 325 TBC layer

configurations on YSZ:Dy

The precision of the previous

results is to be related to the

effects of the input gradient of

temperature on the model. The

sensitivity of the model to the

input surface temperature and

internal gradient for the

configuration (C1) for YSZ:Dy is

shown below. It has been found

that for the usable range of

temperature of this material

(800K–1450K) the equivalent

position remains constant (±8K

error) which allows to retrace

temperature and internal gradients

simply based on Phosphor

Thermometry.

Thermal barrier coatings (TBCs)

are used to protect turbine

components from the extremely

hot gas flow, which may be above

the component materials melting

point. Accurate temperature

measurements enable precise

lifetime predictions, which favor

safety and efficiency. In-situ

monitoring of in-service turbine

components is ideal; a promising

method is Phosphor

Thermometry which uses the

luminescence decay of doped

coatings stimulated by a pulsed

laser. There are various

configurations of candidate

phosphors and host materials,

but it is crucial to ensure both

sensing and integrity needs are

met.

BACKGROUND &

MOTIVATION

METHOD :

LUMINESCENCE DECAY

MODELING COLLECTABLE LUMINESCENCE USING

FOUR-FLUX KUBELKA-MUNK MODEL

INTEGRATION OF DECAY TIME

The Phosphor Thermometry

instrumentation at the University

of Central Florida has been

constructed in collaboration with

Dr. Heeg at Lumium, The

Netherlands, and is composed of

a switchable 355 nm / 532 nm

wavelength pulsed laser that

excites doped specimens.

Neutral density and bandpass

filters are used to collect the

luminescence. A photomultiplier

tube is used to convert the

photons into a detectable electric

signal. The data collection is

then processed through MATLAB.

The sensitivity of the

temperature measurement is

proper to each configuration and

based on the variation of decay

time with temperature. The

equipment has been designed so

it is adaptable to the sample

positioning and portable.

REFERENCES &

ACKNOWLEDGMENTS[1] Fouliard, Q. P., Jahan S. A., Rossman L., Warren

P., Ghosh R., Raghavan S., Configurations for

Temperature Sensing of Thermal Barrier Coatings,

International Conference on Phosphor Thermometry,

25-27 July, 2018, Glasgow, UK

[2] Fouliard, Q. S. Haldar, R. Ghosh, S. Raghavan,

Modeling Luminescence Behavior for Phosphor

Thermometry Applied to Doped Thermal Barrier

Coating Configurations, Applied Optics (2019) -

Submitted

[3] Pilgrim, C. C., J. P. Feist, and A. L. Heyes. "On the

effect of temperature gradients and coating

translucence on the accuracy of phosphor

thermometry." Measurement Science and

Technology 24.10 (2013): 105201.

This material is based upon work supported by the

U.S. Department of Energy, National Energy

Technology Laboratory, University Turbine Systems

Research (UTSR) under Award Number: DE-

FE00312282.

Sensing TBC configurations have

been separated into two

categories:

(C1) is easier to manufacture,

does not add any extra interface

and provides higher

luminescence intensities. (C2)

gives higher accuracy of

luminescence signal [1].

Department of Mechanical and Aerospace Engineering, College of Engineering and Computer Science, University of Central Florida,

Orlando, Florida, USA

Quentin Fouliard, Sandip Haldar, Ranajay Ghosh, Seetha Raghavan

OBJECTIVES

DOPED LAYER TBC

CONFIGURATIONS

Data collection through doped

TBCs at high temperature.

Addition of a PMT with a different

bandpass configuration for the

combination of the decay and the

intensity ratio methods.

Specimen fabrication and residual

strain characterization of the doped

TBCs to ensure the mechanical

integrity of the specimens.

Quantify the luminescence

intensity for any TBC configuration.

Predict the location into the TBC

of the Phosphor Thermometry

temperature output.

INSTRUMENTATION

Fan

Low-Pressure

Compressor

High-Pressure

Compressor

Combustor

Low-

Pressure

Turbine

High-

Pressure

Turbine

& Coated

Blade

Thermal

Barrier

Coating

Image

courtesy: G

E

FUTURE WORK

MATERIALS

YSZ:Eu (1% Eu2O

3, 8% Y

2O

3, 91%

ZrO2) TBC coupons were prepared

by Air Plasma Spray at the Florida

Institute of Technology to validate

initial results of Kubelka-Munk

based models. Er, Dy, Sm and Cr

dwdadw

250

μm

Doped top coat

Undoped top coat

Bond coat

Substrate

(C1) (C2)

Thermally grown oxide

are other

dopants that

will be made

for Phosphor

Thermometry.

This instrument is combined with

an infrared heater (model E4 from

Precise Control Systems Inc, MN,

USA) that is capable of heating the

specimens up to 1300˚C to

reproduce TBC real service

conditions. Measurements have

been taken on YSZ:Eu powder and a

fit allows for retracing temperature.

YSZ:Eu top

coated sample